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Profile consistency: Difference between revisions
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The resulting profiles are known as ''canonical'' profiles. | The resulting profiles are known as ''canonical'' profiles. | ||
<ref>[http://dx.doi.org/10.1134/1.1520282 Yu.N. Dnestrovsky et al, ''Canonical profiles in tokamak plasmas with an arbitrary cross section'', Plasma Physics Reports '''28''', 11 (2002) 887-899]</ref> | <ref>[http://dx.doi.org/10.1134/1.1520282 Yu.N. Dnestrovsky et al, ''Canonical profiles in tokamak plasmas with an arbitrary cross section'', Plasma Physics Reports '''28''', 11 (2002) 887-899]</ref> | ||
This phenomenology is due to plasma [[Self-Organised Criticality|self-organisation]] | This phenomenology is due to plasma [[Self-Organised Criticality|self-organisation]], | ||
<ref>[http://dx.doi.org/10.1134/1.1992581 Yu.N. Dnestrovsky et al, ''Self-organization of plasma in tokamaks'', Plasma Physics Reports '''31''', 7 (2005) 529-553]</ref> | <ref>[http://dx.doi.org/10.1134/1.1992581 Yu.N. Dnestrovsky et al, ''Self-organization of plasma in tokamaks'', Plasma Physics Reports '''31''', 7 (2005) 529-553]</ref> | ||
i.e., the feedback mechanism regulating the profiles (by turbulence) is often dominant over the various source terms. | |||
== References == | == References == | ||
<references /> | <references /> | ||